In the most general case of flow in a compressible fluid the density, viscosity, specific heat at constant volume, specific heat at constant pressure and heat conductivity are functions of pressure and temperature. The solution of equations of motion together with equation of continuity and of energy present great difficulties. The physical conditions superimpose c'rtain boundary values on velocity, density, pressure and temperature. Because the energy equation expresses only in an analytical way the law of conservation of energy with all its possible forms like intrinsic, kinetic, etc. one more restrictive condition must be superimposed on the whole system. This usually contains the thermodynamic relationship between heat added, intrinsic energy and external work. It may refer also to the value of heat content per unit mass. This picture shows that at the present time the difficulties in the solution of equations are probably insurmountable. But it is possible to select cases satisfying only a part of the restrictive conditions, which although uninterpretable in all details from a physical standpoint, are solvable from a mathematical point of view. In the present paper three such cases are solved under the conditions that the coefficients of viscosity and thermal conduction are constant, that only one boundary condition is superimposed, namely the one concerning the velocity at infinity and that all other restrictive conditions are neglected. The cases are: two-dimensional source, circular vortex, and spiral vortex. The solution was obtained in the form of exponential functions and the worked-out examples represent the cases of exact formal solutions of equations under accepted conditions. This last is the main aim of the paper. The obtained results show that from the four parameters two i.e. velocity and density are always interpretable from a physical standpoint, but two others i.e. temperature and pressure are, in some cases, uninterpretable from a physical standpoint. In certain cases they came out to be negative in the whole plane. The case of a source was reduced to adiabatic conditions. Also the case of a three-dimensional source in adiabatic conditions was solved